Visual explanations of machine learning model estimating charge states in quantum dots Yui Muto1 2Takumi Nakaso3Motoya Shinozaki4Takumi Aizawa1 2Takahito

2025-05-06 0 0 630.88KB 17 页 10玖币
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Visual explanations of machine learning model estimating charge states in
quantum dots
Yui Muto,1, 2 Takumi Nakaso,3Motoya Shinozaki,4Takumi Aizawa,1, 2 Takahito
Kitada,1, 2 Takashi Nakajima,5Matthieu R. Delbecq,5Jun Yoneda,5Kenta
Takeda,5Akito Noiri,5Arne Ludwig,6Andreas D. Wieck,6Seigo Tarucha,5
Atsunori Kanemura,3Motoki Shiga,7, 8, 9 and Tomohiro Otsuka4, 1, 2, 10, 5,
1Research Institute of Electrical Communication, Tohoku University,
2-1-1 Katahira, Aoba-ku, Sendai 980-8577, Japan
2Department of Electronic Engineering,
Graduate School of Engineering, Tohoku University,
Aoba 6-6-05, Aramaki, Aoba-Ku, Sendai 980-8579, Japan
3LeapMind, 28-1 Maruyama-cho, Shibuya-ku, Tokyo 150-0044, Japan
4WPI Advanced Institute for Materials Research, Tohoku University,
2-1-1 Katahira, Aoba-ku, Sendai 980-8577, Japan
5Center for Emergent Matter Science, RIKEN,
2-1 Hirosawa, Wako, Saitama 351-0198, Japan
6Ruhr University, Bochum, Universit¨
atsstraße 150, 44801 Bochum, German
7Unprecedented-scale Data Analytics Center, Tohoku University,
6-3 Aoba, Aramakiaza, Aoba-ku, Sendai, 980-8578 Japan
8RIKEN Center for Advanced Intelligence Project,
1-4-1 Nihonbashi, Chuo-ku, Tokyo 103-0027, Japan
9Graduate School of Information Science, Tohoku University,
6-3-09 Aoba, Aramaki-aza Aoba-ku, Sendai, 980-8579, Japan
10Center for Science and Innovation in Spintronics,
Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-8577, Japan
(Dated: December 29, 2023)
1
arXiv:2210.15070v2 [cond-mat.mes-hall] 27 Dec 2023
Abstract
Charge state recognition in quantum dot devices is important in the preparation of quantum bits for
quantum information processing. Toward auto-tuning of larger-scale quantum devices, automatic charge
state recognition by machine learning has been demonstrated. For further development of this technology,
an understanding of the operation of the machine learning model, which is usually a black box, will be
useful. In this study, we analyze the explainability of the machine learning model estimating charge states in
quantum dots by gradient-weighted class activation mapping, which identified class-discriminative regions
for the predictions. The model predicts the state based on the change transition lines, indicating that human-
like recognition is realized. We also demonstrate improvements of the model by utilizing feedback from the
mapping results. Due to the simplicity of our simulation and pre-processing methods, our approach offers
scalability without significant additional simulation costs, demonstrating its suitability for future quantum
dot system expansions.
2
INTRODUCTION
Semiconductor quantum bits (qubits) that utilize electron spins in semiconductor quantum
dots are expected to be good candidates for future qubits because of their high operation fi-
delity and excellent integration properties. Basic operations such as single-qubit[1,2] and two-
qubit operations[3,4] have been demonstrated, and quantum error correction has also been
demonstrated[12] with improved operation fidelity[511]. Furthermore, attempts are being made
to construct large-scale quantum systems using semiconductor integration technology[1320]. It
is essential to trap one electron in each quantum dot to construct semiconductor qubits. Charge
state tuning in semiconductor quantum dot devices is required for this purpose. In previous exper-
iments, this has been mainly accomplished by manually adjusting the gate voltages to achieve the
desired charge states. However, this approach requires a significant amount of time to learn and
execute. This will make tuning large-scale semiconductor quantum systems difficult in the future.
There is a movement to solve such a difficult problem automatically[21]. The main types
of algorithms studied in these methods are script-based algorithms[2427] or machine-learning
(ML) methods[2839]. In particular, ML methods are expected to be more easily applicable to
different experimental environments and more compatible with different devices. Efforts to de-
velop ML methods for auto-tuning quantum device parameters are currently underway [22,23].
In ML methods, the amount of labeled data required for network training is enormous, making
the preparation of labeled experimental data as training data a labor-intensive task. Consequently,
simulations have been utilized to generate training data. This approach has led to the develop-
ment of a method that utilizes the Thomas-Fermi model and deep convolutional neural networks
(CNN) for recognizing charge states [28]. Also, by adding various types of noise that could be
observed in real experiments to the training data, the noise-robust charge states recognition has
been demonstrated [39].
Thus far, charge state recognition has primarily been demonstrated in double quantum dots [28,
31,39]. Looking towards the future large-scale integration of quantum dots, there is a need to
explore scalable methods. Also, while the Thomas-Fermi model with added noise is highly useful
as a physical model, the necessity of such physical accuracy in a data generation model for machine
learning has not been extensively debated. For instance, humans tend to estimate charge states
by focusing mainly on charge transition lines, without giving much consideration to background
noise. Therefore, generating training data with a physical model that reflects these characteristics
3
could lead to the realization of an estimator with judgment criteria similar to those of humans.
Such an estimator would likely be more user-friendly for humans, as it would share the same
criteria for judgment. To achieve this, it is important to clarify the criteria for judgment, which is
usually a black box.
In this study, we analyze the operation of the ML model that estimates the charge states in
double quantum dots. We propose pre-processing the data through binarization, which enables
us to use a simple simulation model to generate training data. We also visualize the interest of
the model by gradient-weighted class activation mapping (Grad-CAM) [40] and confirm that they
are on the charge transition lines. By incorporating feedback from the Grad-CAM results, we
demonstrate improvements in the ML model.
PREPARATION OF THE CHARGE STATE ESTIMATOR
Figure 1(a) illustrates the process flow for generating a charge state estimator (CSE). Initially,
the preparation of training data is needed to train the ML model. We utilize a constant interac-
tion (CI) model in the simulation for simplicity, where quantum dots are modeled as a capacitor
circuit[41,42]. Using this CI model and treating the electrostatic coupling between the double
quantum dot and the charge sensor, we can obtain the charge stability diagrams with the size
(30×30) pixel measured using a charge sensor by changing the parameters in the model. This size
is chosen to achieve a sufficient resolution to distinguish the charge transition lines. The next step
is to prepare the charge state label: no quantum dot (ND), left (LD), center (CD), right (RD), or
double quantum dot (DD), for each stability diagram (Fig. 1(a) step 0). Note that the CD state is
formed by strong coupling between both dot sites, which in the CI model is expressed by setting a
large value for Cm. Here, the diagrams are automatically categorized based on the largest number
of quantum dots in the region.
Next, pre-processing is performed on these images. All images are differentiated in the x-axis
to make the charge transition lines clear (Fig. 1(a) step 1). Then, the images are binarized by
adaptive thresholding to simplify them into black and white images (Fig. 1(a) step 2). Here, the
charge transition line is set to white, while the background is set to black. In this process, we use
Adaptive Thresholding by the OpenCV module [43].
To adapt to noisy experimental data, random noise is added to these images. Due to binarization
in the previous step, noise can be realized by simply flipping the black and white pixel values at
4
摘要:

VisualexplanationsofmachinelearningmodelestimatingchargestatesinquantumdotsYuiMuto,1,2TakumiNakaso,3MotoyaShinozaki,4TakumiAizawa,1,2TakahitoKitada,1,2TakashiNakajima,5MatthieuR.Delbecq,5JunYoneda,5KentaTakeda,5AkitoNoiri,5ArneLudwig,6AndreasD.Wieck,6SeigoTarucha,5AtsunoriKanemura,3MotokiShiga,7,8,9...

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